Program Information
Towards An Optimized 3D Scintillation Dosimetry Tool for Quality Assurance of Dynamic Radiotherapy Techniques
M Rilling1,2,3,4*, M Goulet3 , S Thibault1,4 , L Archambault1,2,3 , (1) Département de physique, de génie physique et d'optique, Université Laval, Quebec City, QC, Canada (2) Centre de Recherche sur le Cancer, Hôtel-Dieu de Québec, Quebec City, QC, Canada (3) Département de radio-oncologie, CHU de Québec, Quebec City, QC, Canada (4) Center for Optics, Photonics and Lasers, Université Laval, Quebec City, QC, Canada
Presentations
SU-D-213-3 (Sunday, July 12, 2015) 2:05 PM - 3:00 PM Room: 213
Purpose: The purpose of this work is to simulate a multi-focus plenoptic camera used as the measuring device in a real-time three-dimensional scintillation dosimeter. Simulating and optimizing this realistic optical system will bridge the technological gap between concept validation and a clinically viable tool that can provide highly efficient, accurate and precise measurements for dynamic radiotherapy techniques.
Methods: The experimental prototype, previously developed for proof of concept purposes, uses an off-the-shelf multi-focus plenoptic camera. With an array of interleaved microlenses of different focal lengths, this camera records spatial and angular information of light emitted by a plastic scintillator volume. The three distinct microlens focal lengths were determined experimentally for use as baseline parameters by measuring image-to-object magnification for different distances in object space. A simulated plenoptic system was implemented using the non-sequential ray tracing software Zemax: this tool allows complete simulation of multiple optical paths by modeling interactions at interfaces such as scatter, diffraction, reflection and refraction. The active sensor was modeled based on the camera manufacturer specifications by a 2048x2048, 5 μm-pixel pitch sensor. Planar light sources, simulating the plastic scintillator volume, were employed for ray tracing simulations.
Results: The microlens focal lengths were determined to be 384, 327 and 290 μm. A realistic multi-focus plenoptic system, with independently defined and optimizable specifications, was fully simulated. A f/2.9 and 54 mm-focal length Double Gauss objective was modeled as the system’s main lens. A three-focal length hexagonal microlens array of 250-μm thickness was designed, acting as an image-relay system between the main lens and sensor.
Conclusion: Simulation of a fully modeled multi-focus plenoptic camera enables the decoupled optimization of the main lens and microlens specifications. This work leads the way to improving the 3D dosimeter’s achievable resolution, efficiency and build for providing a quality assurance tool fully meeting clinical needs.
Funding Support, Disclosures, and Conflict of Interest: M.R. is financially supported by a Master's Canada Graduate Scholarship from the NSERC. This research is also supported by the NSERC Industrial Research Chair in Optical Design.
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